Sonar simulator



NOV. 14, 1961 F. A. LINDLEY, JR

SONAR SIMULATOR Nov. 14, 1961 F. A. L1NDLEY, JR

SONAR SIMULATOR Fiied Nov. so, 1954 8 Sheets-Sheet 2 WWI Nov. 14, 1961 Filed Nov. 30, 1954 F. A. LINDLEY, JR

SONAR SIMULATOR 8 Sheets-Sheet 3 OUT/00725 7'0 RANGE A 77E/VHA TVO/VMFL /-/ERS vaar/zur TIL 7' ERROR 8 Sheets-Sheet 4 F. A. LINDLEY, JR

SONAR SIMULATOR Nov. 14, 1961 A. LlNDLEY, JR 3,008,244

SONAR SIMULATOR Filed Nov. 50, 1954 8 Sheets-Sheet 5 ARGE? QBDRESS/O/V 5575 f7 E j i @AA/66 052A Y 4H NOV- 14, 1961 F. A. LINDLEY, JR 3,008,244

soNAR SIMULATOR Filed Nov. 30, 1954 8 Sheets sheet 6 CORRESPOA//A/G ASPfCT Nov. 14, 1961 F. A. |ND| EY, JR 3,008,244

soNAR SIMULATOR www? l I l l I i P//Lsf /A/pur.

3,008,244 SONAR SIMULATOR Frederick A. Lindley, Jr., Flushing, N.Y., assignor t Smith-Meeker Engineering Company, New York, N.Y., a corporation of New York Filed Nov. 30, 1954, Ser. No. 471,987 Claims. (Cl. 35--10.4)

invention relates to a sonar trainer and particularly a device for generating :and controlling simulated signals -to accord with the aural .and visual characteristics of echo land transmitted signals associated with standard sonar gear.

rIlhe invention embodies a signal simulatin-g device which is adaptable .to various types of sonar gear. This is due to 'the fact that no elfort is made to simulate the gear itself lbut only the characteristics which are thought to have prominence in every returning signal. Nor is the simulator limited to any specified number of assumed targets, or the simulation of any particular characteristics deemed from present studies to be most significant in the composition of sonar echoes. The signal modulating voltages are synthesized in separate, unitized circuits which results in a highly ilexible design and the possibility of removing or replacing control units depending on the degree and kind of realism it is .desired -to achieve.

Generally there are rtwo fairly distinct aspects of sonar simulation, one being the lgener-ation of .the basic signals, such as reverberation, target and wake, and the other control of the ysignals in accordance with target motion and relative position. Most of the circuit features are readily adaptable to various types of sonar gear and have additional advantages which will become apparent on reading the detailed description.

In the target motion section of the simulator applicant has so arranged the units that the various control voltages are derived from a common multivibrator pulse producer. Hence the simulated generation of the target envelope, target wake envelope, a Adelayed pulse for target depth echo and acontrolvoltage, which imparts aspect position characteristics to the target and wake signals, originates at a single source. 'I'his insures stability and al consistency in operation and makes for simplicity in construction'and maintenance.

Furthermore, unique circuitry is presented for phase shifting the output in the .four channels which carry the target, wake and other echo signal-s to the four transducerquadrants in the operational gear section. A plus or minus 90 shi-ft is realized without Ithe necessity of gauging the -shifter units or unrealistica-l-ly modul-ating signal amplitude. frequency shift to 90 has been especially designed for the simulator and is an improvement over deflection limiters in use.

In recognition of the fact that changes in the' aural andl visual appearance of the signals occur with changes in ping length, the invention provides means for impressing on the signals random frequencies which are controlled by the operational gear :as afunction of ping length. A morerealistic presentation of the reverberation,l wake andtarget signals is accordingly effected.

-Afunique system is provided for controlling shift in frequency to simulate doppler effect as produced by own ships movement and for applying the target doppler voltage for moving targets to the target oscillator as a function of Atarget pulse and transducer train angle all of which represents an advance over present systems.

VThese and other novel features with respect to t-he arrangement of .the simulator uni-ts and circuitry will be appreciated on reading the detailed description which follows, in which Also the circuitry for limiting the ice FIG. 1 is a partial block diagram of the sonar simulator;

FIG. 1A is a block Idiagram showing an individual target section. IFIGS 1 and 1A comprise a complete Y single target simulator;

FIG. 2 vshows the circuitryfor phase limiting;

FIG. 3 is a block diagram showing a unique system for producing own ship and target doppler elect;

FIG. 4 shows circuitry for bearing error positioning;

FIG. 5 shows circuitry for bearing and depression angle gate control;

FIG. 6 vshows a typical voltage pattern for a CT rotor, a transformer in series therewith and a combination pattern as .the rotor is rotated through 360;

FIG. 7 is a circuit scheme for producing a linear .time delay as a function of range in triggering a multivibrator;

FIG. 8 shows the time relation of the transmitter pings and the delayed pulses;

FIG. 9a shows the evolution of wave forms in the production of the target envelope wave form;

FIG. 9b shows the effect of clipper input amplitude on the duration of the target envelope pulse;

FIG. 10 shows the relationship of target aspect and the simulated ytarget aspect deflection voltage;

FIG. l1 shows the circuitry for producing signal controls Ito simulate target and wake position characteristics;

FIG. 12 shows a Z voltage wave form and the relation of target yaspect angle to its tangent; and

FIG. 13 is a lgraph of the tandem potentiometer output as compared with the tangent function.

The echo -signals which are returned to a sonar receiver from 'targets in motion and :their resulting wakes and from other objects situated in a random fashion throughout the sea volume are all basically related. That is, their fundamental wave form component is basically the frequency of the transmitted sound pulse. The device therefore employs a 'single oscillator 10 for the artificial generation of these signals. Hence there is no problem of maintaining separate oscillators at lthe same basic frequency which is frequently a sou-rceof trouble in other sonar trainers in yview of the fact that the ear positioning and can distinguish differences land changes of only .a few f lIf it is desired to correct the oscillator frequency cycles. to `the frequency of the sonar transmitter lduring transmitting intervals, a frequency error corrector 12 may be provided as illustrated generally in FIG. 1. A system for stabilizing frequencies is disclosed in lmy Patents Nos. 2,688,730 and 2,528,632 and could be appropriately adapted to the present sonar simulator.

It is recognized that target, wake yand reverberation echoes resulting from short transmitter ping lengths give rise .to a less distinct tonal characteristic than echoes from longer transmitter pings. The shorter the transmitter ping length the more intense the random phase and amplitude variations of the echoes appear to-be and conversely the longer the transmitter ping length the less intense the randomphase and amplitude variations of the echoes appear to be. In order to realistically impart this condition to the simulated echo signals, a wide band random noise generator 14 is provided which is connected to a noise modulator 16 through a filter 17 which is adapted to select a wide frequency band in the vicinity of the oscillator or transmitter frequency. To the noise modulatorA 16 is also connected the oscillator 10. The amplitude of the random noise fed to the noise modu.- lator 16`is controlled from the operating gear section as a function of ping length. The noise modulator 16 out-l put is fed to a target envelope gate 18 and a reverberation envelope modulator 20 which in turn furnishes reverberation signals and also wake signals to a wake gate 22. The modulator 20 has a low pass RC filter 23l which Patented Nov. 14, 1961:

aoosgea selects only a very low, baud of random noise frequencies thus imparting common random envelope character-4 istics to the wake and reverberation signals. The noise modulator 16 furnishes the fundamental wave components for tar-get, wake, and reverberation and consequently by varying the degree of noise modulation the change in tonal effectA may be'imparted to all types of echo signals as though there hadA 'been a change in. transmitter ping'Y length. This method of varying thejt'onal effect and visual appearanceY of' the echo signals is,v consistent'V with the theory that the degree ofrandonrmodulation largely'determines their character; especially true where the transmitterlpings lengths. are short. YThe ping length attenuator control connectionto the noiseimod'ulator 16 as shown in' FIG. l'venabl'es the.

operator to control the change in Vsignalz'elect, with change in ping length. i s Y The three signal outputs target signal, walexand re-V verberation can beV branchedout for the addition`` of as many echo signalsY as desired.'v Thus if.' three targets,

are desired the signal output from the noise modulatorV 16 is fed to three target' envelope modulators. The generation and control of the. three individual' target envelopes is accomplished in accordance with the'three individual targetv motions, and when 'fed to their respective target envelope rno'dulatonkeys` orl gates on aA corresponding echo signal.

This has; been found to be normally keeps the target speed voltage disconnected from the reactance modulator input line and thus own Ysljips speed voltage is in control of the reactance modulator. However, when a target envelope and a target depth echo envelopepulsevis applied to the Vtarget gate in box 18 it switches forthe durationV of the pulse. the target speed voltage (to the..doppler' reactance Vmodulator input line.:4

Impedances are arranged sof that the-targetfrelative speed voltage sets theline voltagewhen it isclampedj to it. The

impedance of the target relative speed voltage-source isconsiderably lower than the impedance of the own ships i speed voltage source. The action is to momentarilyrshift the signal, oscillatorfrequency to correspond to the target doppler. Target envelopes gate Vin box V1,9,.connetzts,

If it is desired that thesev three vsignals have wakes= theV signal output for Vwake from the reverberation envelope Y doppler' effects. A positive voltage would forexample.y

shift the frequencyr higher andza'" negative voltagev shift it lower;

Since sonar gear'. observes doppler Vefectsf in" stationary objects due toV own ships speed, the'simulator provides for own ships doppler by supplying a proper control'vol'tage to the. doppler modulator Z4. AnA.C.. voltage pro'- portional to speed is provided. Reverse' speed would ,be represented by reversing the phase YorV polarity. The amount of doppler depends also onthe angle of train of the transducer with respect to the stationary target'. A cosine-potentiometer in ybox 26 excited by the A.C.'vojlt age, and operated. by the train angle, ofthe transducer furnishes the cosine component'. The cosine potentif ometer also is arrangedtoreverse the phase or polarity when the train angle is Ypointed aft to correspond' with the actual reversal of` own ships doppler When'sWingingthe; transducer trainingA from.. forwardY to` aft and 'vice-versa.

This cosine component `is their` rectified by' aj differ-`V ential rectifier in lbox 26. The,diierentialrectifier is capable of giving either a positive or negative';D.C.jvolt ageV output depending; on the A.C. phase'or polaritycorrespondingto theforward or reverse speed', This'is followedlby" a filter, also in box 26, to give aA smooth.D;C. output. with this output. The resulting D.C. voltag'eis' ,continu--Y ouslyu applied andV controls the..,reactance modulator for own ships doppler.

Each target relative speed voltage, on the sa'ine-Vcali-fM A highvalue of resistance 'is` placedE in series,A

fc5 Y as well. This A.C.'voltage 1s introduced" 1n serresfwith, Ythe rotor windings. At the other endY of the rotory Wind- Y ingsI the resultant addition ofithisvoltage and thereto!" the target envelopeY generatorsptov the. targetjgate' inf-box 18 `and the target'envelrope clampY in box y30. *It Yis controlled by the train and tilt angle of thetransducer. The

envelope pulses, which are passed by th'elargestenvelopesA gate in box 19, gate onlthe target' signa-l' in box 18 and also the target yrelative 4speed voltage in Y.the target envelope clamp permitting it" to be applied `to theV doppler'r modulator. 24. Thusi in'the sameA Ytime .interval `the tary.` Vgetdo'pplerVY effect is applied to theV signalalong with the gating of the target signal to the transducer ichannels.VV

The provision for preventing passage, of thatargetand wake signals to thetransducer channelsand theV target Doppler voltage to thereactance modulatorexcept when the transducer is trained` nearly on the targetis illustrated in FIG. 5.. A The gating must bemaintained closed'whenthe`V transducer is' olf-train in either"v tilt or'train angle' or both. As shownlinV FIG. 1A the target' gate 118,' wake gatey 22 and target Dopplerr'clarnp 30 are'supplied kby'rectiiiers inl b'ox 25 with a bearing and tilt' olf-train `error control voltage'. This error controllvoltage is derivedi from the bear'- ing andl depression angle gatecontrol circuit of FIGQ'S". y

Two CT synchros. 54: and 731, (FIG. 5) are excitedA bye. transducer tilt angle synchro generator (not shown) and` a transducer trainangl'e vsynchro generator 33" (1:10.41Y

whichhave their rotors 56 and" 32j respectively, turned'as.

a function of assumeditarget depression angle and target relative bearing respectively. The azimuth angle servo. system islocated in boxZTwhile thel depression ,angle-r servo systemlis .located in Ybox 28'. Y

Oneiwinding of' each rotor is connected thedepres.- 1 sionV andazimuth off-train error differential rectiiiersin box' 48; The other winding of each rotor,V whiclris.Ori-r ented 90 from its associated windingfontherotonis con:V

nected each to aseparate cathode offdiual rectitiertubes j 64v and 65 in, box 25 andto furnish subsequently the gate control' bias. The same windingwhich supplies the,-Y

winding is employed.r In the interest `of clari'ty, the1rotorf in FIG. 4.

windings for the gating rectiers'64 and 65 arenotslijowinv @A cycle trarisformerzsupplies,V from the' synchro` buss' anv A;C. voltage" just equal Vto .the maximumV rotorl v voltage and has its'Y phase carefully adjusted for a O. or

bration basis as own ships speed, is fed to its. individual"` I 30. This acts as a switch between the target relative speed control voltage; andi the reaetance: modulator-input `It relationshipto the rotor voltage depending upon the selectedfnull position;V The synchrosare uniform enough, Y

inV manufacture so that thisg-oneftransformeran. supply` not only both CT'synchrosrbutjthose, for all otherQtargets voltage is'rtaken out.

Y The normal CT rotor voltage describes a figure-.of eight` patternfwhenrevolvedfthrough`3-60. It shows two nulls ofl voltage 180 apart and the phase,l ofthe two loops of voltage differ byv 180". Curve 1 shown in FIG;V 6j illustrates this voltage pattern. Y lThe transformer,"sincev it sup'- plies a constant A.C.' voltage Vregardless vofiiC"l"ro'tation,

Y l It is therefore to removeV Y this ambiguous null that thev circuitv of thisV second 9f0`1 can be represented by a circle, curve Z, its radius being equal to the maximum of the figure of eight pattern. Combining these two voltages by addition results in the cardioid pattern shown by curve 3. This cardioid pattern has only one null which occurs when the out of phase maximum figure of eight voltage just balances out the steady A C. voltage of the transformer. For all other rotational positions a resultant voltage occurs. It will now be noted that this cardioid null is 90 removed from the figure of eight nulls and therefore would be coincident with one of the two 180 nulls of the first rotor winding. By this means the ambiguity of the two rotor nulls is removed.

The combined rotor output is passed to the cathodes of the dual rectifier tubes 64 and 65 for each of the two CT synchros respectively. The two plates of the rectifiers are joined and feed a common filter 66. The output of filter 66 is fed to the target envelopes gate in box 19 for controlling the target envelope clamp in box 30 and the target gate in box 18 and the target wake gate in box 22. The result is that if the transducer is off-train in either tilt angle or train angle or both a rectified negative voltage is produced in the filter. Therefore, in order for the gates to be opened by removing the negative voltage, proper training on the target for both bearing and depression angle must occur.

There is an important additional characteristic not yet considered. Where an AN/SQG-() transducer system is employed, the echo signals feed into four elements of the transducer which receive the signals in slightly difierent phase relation unless they come from a point source or the transducer is directed squarely at the object in both train and tilt angle. If now we train slightly off, say in azimuth, the phase of the signal should advance equally for example in the two left transducer channels and correspondingly retard in the two right transducer channels. Differential bias or position voltages applied to the respective transducer channel phase Shifters accomplishes the simulated phase modulation.

The differential or position error voltage is obtained by comparing synchro information differentially as explained with reference to FIG. 5. The outputs from the rst rotor windings of the two CT synchros 54 and 31 as described are fed respectively to the depression angle error olf-train dierential rectifier and the azimuth error off-train differential rectifier. The outputs of the differential rectifiers represent positioning control for top, bottom and left, right. By combining these voltages in a resistor network appropriate control functions for the four transducer channels top left, bottom left, top right and bottom right are obtained. Four phase Shifters in box 150 are employed to modulate each of the inputs respectively in the four channels TL, BL, TR, and BR to the transducer. Since each target with its associated wake is a separate control function this circuitry is repeated for each target as can be seen by reference to FIG. 1A.

FIG. 4 illustrates the basic bearing error positioning simulation means employed in the simulator. CT synchro 31 has a rotor shaft 32 the position of which represents the targets relative bearing. Its three-phase stator is connected to a three-phase stator of synchro generator 33 by leads 34, 35 and 36. Rotor shaft 37 of synchro generator introduces azimuth angle of train. Obviously when target position and azimuth angle of train are equal a null of CT rotor voltage will occur. Plate rectifier tubes 40 and 41 in box 48 have their grids connected push-pull to the rotor through transformer 42. Balancing potentiometer 43 in the cathode circuits of tubes 40 and 41 assures equal voltage output to the phase Shifters when no A.C. signal is applied to the grids of the rectifier tubes from the CT synchro 31. Thus with equal voltages applied to the phase Shifters the degree of phase shift is the same in each so the phase of the signal in the left side is the same as that in the right. The AN/SQG-() sonar interprets this as proper zero error training on the target.

The voltage applied to the plates of the plate rectifier tubes 40 and 41 is 60 cycle A.C. from the synchro A C. buss. It is applied to the two rectifier tube plates through equal load or plate resistors 414 and 45. Thus with no grid signals and the cathode potentiometer 43 balanced equal plate rectification takes place as mentioned before. When a signal voltage from the CT synchro, due to an off-train error, is applied to the two grids in push-pull, through transformer 42 the grid voltage in one rectifier will be in phase with the plate voltage while in the other rectifier the grid voltage will be out of phase with the plate voltage. This causes increased rectified plate current in the one and reduced rectified plate current in the other. A larger off-train angle resulting in a larger voltage on t-he grids increases the current still more in the first tube and further reduces it in the other.

If the off-train angle is changed in the opposite direction, the 'CT voltage would change 180. This interchanges the grid voltages producing the reverse differential rectifier effect. The rectifier tubes outputs are limited either by cut-ofi or grid current depending on the polarity of the grid voltage.

The outputs of the differential plate rectifiers 40 and 41 are filtered by resistor 46 and capacitor 47 and resistor 46a and capacitor 47a respectively. This assures a smooth D.C. control voltage to the phase Shifters.

The same technique which was used for producing a simulated phase control differential effect in accordance with the bearing off-train errors of the target, is employed for tilt angle errors. The resulting four biases which bear a proportionate relation to train and tilt errors are applied to the target phase Shifters to Shift the signal relative to the center of the four quadrants of the transducer.

All echoes must be presented in a proper time relationship with respect to the transmitted pulse depending upon their range. For this reason these circuits have to be timed or synchronized from the AN/SQG-f) sonar, or other type sonar in use. This is accomplished by bringing into the simulator pulse No. 1 which is coincident with the leading edge of the transmitter pulse and initiates the range time, and pulse No. 2, which iscoincident with the end of range time, initiates the recycle. These two pulses drive iiip flop timing multivibrator 64A. T'he multivibrator wave form output furnishes opposite polarities for subsequent circuit requirements.

The wave form polarity which has the negative swing during the range time is used to drive a linear sawtooth generating circuit in box 66a. This linear sawtooth voltage is branched to as many targets as necessary. T-he use of a common linear sawtooth voltage source for all targets makes for alignment simplicity since a linearity calibration is made only once and is the same for all targets.

This sawtooth voltage is employed by the simulator to determine range 'which is referenced from each transmitted ping in terms of time delay. A circ-uit for obtaining a pulse at some time delayed interval as determined from positional information is illustrated in FIG. 7. A resistor 67 is excited with a D.C. voltage of negative polarity by potentiometer 68. This D C. voltage is a linear function of range. To a second resistor V69 in series with resistor 67 is applied the positive'rising sawtooth voltage. A target trigger circuit 70 is connected to the junction of the two resistors and is adjusted to fire at the time the voltages reach zero, when it generates a time delayed pulse corresponding to the time it takes the sawtooth voltage to rise to the zero value at the junction of the two resistors. The relation of the three waves are illustrated in FIG. 8. Zero voltage of course occurs at the junction of the two resistors when the positive rising sawtooth voltage exactly balances the negative D.C. The resulting pulse is coincident with range, being generated at a. specified time subsequent to the transmitted pulse. As shown in FIG. 1 the range Y lined predeterminedv duration.

In-practicek the duration ofthe target echo pulse corresponds tothe length of the targetin range. That is, the duration is longest when theV target presents a fore to aft aspect and shortestV for bea-m aspect. -On the otherV hand, ther intensity or amplitude of the4 target echo` is greatest in beam and' smallest for fore and aft aspect. The generation of simulated target aspect voltages andy the. control of the target envelope as a function of` target:

aspect, depth echo and wake simulationY are all'derived fromthe target control multivibrator 75 andi are effected ini a unique combination of interdependent electronic.

units, Y

In target ZV voltage generator box 76 a ZE shaped' wave.

having equal'` amplitudes each side yof the A.C. axis is t formed by employing the pulse from Ythe target' control multivibrator (wave form'A in FIG..9) to generate a sawtooth voltage (wave form B) which is'recombined` with the multivibrator pulse to produce the Z 'voltageV (wave form C). This wave form is clipped in. targetren-V velope. generator `box 78 '(wave formy D )f and'thenk diierentiated` (wave form E) resulting inl a center pulse Whose mid-point of duration corresponds to the center of the original Z voltage. The negative leading and trailing pulses respectively are' then clipped off leavin-g only the center positive one (Waveform F) which isy employed VVas the target envelope. f

By suitably controlling the amplitude of the Zvoltage ina Z voltage generator 76 as a function of 'target aspect wevprqduce a Vproper duration variation'of this target envelope. Additionally it will be observed that the am-V plitude. of theV dilerentiated pulse will vary. With a large amplitude ofZf voltage. resulting: in a short duration of the pulse We get a proportionate increase in the amplitude of the! pulse. This it'will beobserved corresponds toa beam position of the target. sol-we also obtain the simulation of tar-get intensity increase 'with beam aspect to which this duration'of shortest pulsev would correspond. Y Y

Where the target presents ay fore.l andA aft aspect, the

' amplitudefofY the' Z Voltage input is'reduced resulting in a. differentiated pulse of longer-duration. See FIG; 9b. The 'amplitude of the diierentiated'pulse is` small which rellects the' actual state of target echo intensityV as comf paredfwith beam. aspect.

Innad'clition to form the. target envelope the'Z voltage is; employedY to generatea target aspectvdeecti'on voltage which, when fed to the target phase Shifters produces By .refening tothe diagramrof FIG. 10,` we see howf this Z voltage must -be cont/rolled so asv to convey the proper aspectrepresentation: Y As pointedfout the duration of, the:- Z voltage or its lengthy in'range. is at all'ftimesa constant, therefore We seetheproper control is only one of, amplitude and polarity; Position `1.v which is target Ythe duration of the oridinal Ztvoltage.

neously, interference resultsfvvhiehzv destroys the. aspectv presentation. Y It' therefore'. shows as only a blob. This:

representation is accomplished by switching ofi the Z. volti age just before 90 aspect is reached. j The Zvoltage'remainsyoiuntil a corresponding position a;Y few degrees past 90is. reached, whereupon ltheZ voltage is switched on but lthis time with thelreversepolarityas noted from positions a to b position; V3'. .The Z vol-tageisjnovv-y reducingposition 4' until it reaches zero value at an aspect of 180, showny by position 5.:

with the polarity and amplitude Vcharacteristic Vinturning from the Oaspect position; Thus itwill benotedathalt Y.

the sequence of-v Z voltage variation. -goes through two cycles for every 360 of target aspect rotation.

By selecting' the corresponding. and. appropriate polarity of the 'Z voltage asfa function ofzthisltarget aspect wecan select the positive half cyclefas occurringzbeforeY or after correspondingrto theV targets stern being before or after;Y

By clipping'and selectinguthe Vpositive Zvoltage polarity i' Y an envelope iss-obtainable.. Thiscan be used"as:the:wake

envelope and is able, to? properly? position the` wake before'` orafter the. targetv depending' upon'the targets direction of'travel..V It gates on thewakesignalin the. wake gate box 22. When the target is inthe beam position the t AN/SQGT( )A sonar` cannotv present target wake Vsince it would be simultaneously received with the-target.Y This fortunately occurs during the polarityswitchover so Vthe, wake envelope is, appropriately removed duringthis, aspect position j 'f This wake envelope isof xed duration depending upon.` It presents' no serious problemhowever, for whichth-e AN/SQG-t) wakes WouldquicklyV runfoifthe limited visible. viewing sector and additionally,'wakeV intensity variationswith t speed are far more significant. This intensity Yvariation aspect at 0 shows the voltage-at thenecessaryr zero. am-

Furrther turning of the target. requires increast the sawtooth voltage.

of thewake signal is providedfforso very'little'lossroffl significantwake simulationy will occur and the simplicity 1 of thefxedj relationship'isvery real and desirable.V

' The target; depth echo occurs onV submerged targets only during the beam intervalKofaspect.: Itr'actually isa multiple echo of thetargetproducedby signals being-rellected the; preceding Atarget motion functions is. again usedY to; generate the target .depth echo envelope. `Here thefsaw;

tooth voltage isemployedl to furnish a time'rdelayedfpulse a inl a coincidence circuit.- The amountof tim/edelaytis affunctonof a'DpC. voltagefrom a potentiometer whichl inv-turn VVisrotated 'as-a function of targetdepth. 'f The sawtooth 4voltage and the potentiometer 'voltageare'Y fso' proportioned that zero depth position gives a pulse coincident with that. of the target which would'be themid'dleA of the sawtooth voltage.

Increases in depth wouldjin-r creasingly ydelay the coincidence pulseupfto. the` limit of,

` Ifan adeqpate'duration orig-- inally selected sutlicient depth positioning will benavai able.

voltage generates-a pulsefina pulse lforming circuit which is used as the targetdepth echol envelope; in target depth echo envelope box. 8,0.'v Since 'thisy depthvechoaonlyv occurs in the target beam position it doesnot have to-.have any*` f variation in its Yduration with.` respect-to: target aspect.

" However.; it necessary.. to. switch'it off? for all target aspect positions'except thebeam` position` vThisnecessary control is fortunatelyv readily available from the target aspect deection box89. Because the'. depth echofis gen erated from thejtai'getv Z voltage :generaton it moves: along` After passing through Y 180 the Zvvoltage agairr'increa'ses butwith 'afreversed polarity'.` This, it' should .be noted, corresponds exactly' The. coincidence of fthisfdepthy voltage and the in4 range with the target, differing from it only as a function of depth.

Since all these various target motion characteristics are derived from the one range control function it will be seen that a high degree of stability in their relationship as respect to range is to be expected.

It is thus seen that the generation of target, target wake and target depth echo envelopes and target aspect deection voltage are derived from a target multivibrator 75 which generates a wave form with a fixed predetermined duration initiated and controlled by the range coincidence pulse. The duration of this wave form is selected on the basis of a minimum target range compromised with the selected distance over which it is desired to display wake. This might be set up as an example employing 'round numbers. Assume a target 300 lfeet in length and positioned with a bow or stern aspect so that its length is fully displayed in range. Thus the duration of this ymultivibrator pulse mustpbe for a minimum distance of 300 feet, which is plus and minus 150 feet either side of center. The bowror stern, whichever end is facing us, would correspond to and be very close to the initiating coincidence range pulse. The minimum position this coincidence could take Would be at the beginning of the linear sawtooth voltage corresponding to a zero range. The bow or stern in this example would also be near this zero range but the center would be 150 feet away.

If we now decide to lengthen this target multivibrator wave form by an additional 400 feet or 200 feet on each end, the nearest we could bring the bow or stern of the target ship to zero range would be 200 feet. 200 feet then would-represent the minimum range of the simulator.

Thus the total length of the target multivibrator wave form is 700 feet or 350 feet either side of target center. It allows us to present wake for a distance of 350 feet before or after the target as measured from the center of the target. j l

This one shot multivibrator'wave form when triggered, h olds itsposition for a predetermined period then drops back. Referring to FIG. ll the adjustment of the duration of the multivibrator return swing is accomplished by an adjustment of the grid time constant by variable resistor 85. The output of multivibrator 75 is connected to the grids of two m'odes 86 and 87 being coupled thereto by capacitors 8S and 89a. Tube -86 has its cathode grounded and is a sawtooth generator switch tube which produces a sawtooth voltage during the interval of the Wave form when the tube 86 is switched oil". Tube 87 is also cut-off by the multivibrator negative swing but has an adjustable biasing potentiometer 88a which is connected to its-grid to allow the tube cathode voltage to be set during its conducting interval between negative swings. This as will be seen is the base line `for the Z voltage.

Tube 90 associated with tube `87 has a common cathode connection' and its grid in turn is directly coupled to the plate of the sawtooth switch tube 86. This direct connection is used to maintain D.C. levels.

The action of the circuit is as follows: The second tube 87 during the interval between pulses draws a current determined by its bias setting potentiometer 88a which sets the voltage of Ithe common cathode junction. The third tube 90 during this .interval has the low plate voltage of the switch tube on its grid and is therefore non-conducting by virtue of its positive cathode. When the pulse anives the second tube 87 is cut oit leaving the third tube 90 alone to control the cathode voltage. Since this tube now acts as a cathode follower it repeats the sawtooth voltage applied to its grid. At the end of the pulse and sawtooth the second tube 87 regains control of the cathode voltage and sets the base line. By adjusting the bias of this second tube 87 the base line can vbe set at the middle of the sawtooth voltage with the result that the wave -form of voltage at the cathodes is the symmetrical Z voltage described.

The Z voltage is taken oiv through two connections. One directly from the cathode where the voltage is constant, the other from the arm of potentiometer 91 which makes up the cathode load resistor and thus supplies a varying output depending on the potentiometer position.

A capacitor 92 connects the cathode of tube 90 to the grid of tube a. Tube 90a is connected by capacitors and 100a to potentiometer 93 which is excited by its push-pull output. Potentiometer 94 has its two end terminals connected to the arm of potentiometer 93. The potentiometers 93 and 94 have continuous rotation with a l5 to 20 degree gap at the ends of the winding representing beam aspect. They are grounded at their center taps by leads 97 and 97a. This corresponds to fore and aft aspect as previously explained. The rotating contact arms of the two potentiometers are mechanically coupled together in the same positions and are rotated as a function of target aspect at twice speed. The output of the two cascaded potentiometers supply a voltage which varies with potentiometer rotation and has in addition a proper polarity for target aspect deflection, see FIG. 12. The voltage output is used to modulate the phase Shifters differentially or in push-pull so as to impart to the echo signal a corresponding phase positioning.

The wave form of FIG. l2 has a xed duration so that t which represents the time of a 1/2 cycle will always be a constant. The -function the potentiometers must provide then will be to establish the relationship of the peak voltage e with respect to the aspect angle a. This can be readily discerned by considering the solid line wave form of aspect angle a and voltage amplitude e and the dotted line wave form representing a different aspect angle a and its corresponding voltage amplitude e.

Observation discloses that the tangent of the aspect angle a involves the time t and the voltage e. Thus tangent a equals e/t for the solid line wave form and tangent a equals e'/t for the dotted line wave form. Since t is constant for both cases the relationship of the voltage e to the aspect angle a is as the tangent of the aspect angle.

This requires that the output aspect deflection wave form vary in amplitude as the tangent of the aspect angle. Sine functions are readily obtainable in potentiometers of standard manufacture but tangent functions are not. The tangent of an angle varies from zero at 0 to iniinity at 90. This is obviously an impossible function to reproduce and therefore for practical reasons we have lto stop short of 90. Fortunately we do not have to go to 90 because this represents the beam aspect position of the target where the aspect degenerates. Thus actually we have to stop a few degrees short, approximately 5 or l0 degrees. The value of the tangent function is 5.67 for 80 and 11.43 for 85 representing reasonably achievable values.

A potentiometer wound to reproduce a tangent function up to a reasonably selected value would be quite a special item. While this could be done it was deemed a far more desirable situation if it could be accomplished with more standard potentiometers. A suciently accurate method fortunately exists, using cascaded linear potentiometers.

The two linear potentiometers 93 and 94 are arranged to have continuous rotation and the gap between opposite ends of the -windings is about l5 to 20 degrees. When the contact arms passes over these gaps the circuit is obviously opened and this position represents beam aspect, all deflection voltages being removed. Opposite the gap or at the midpoint of the winding, a tap is placed and this is made a grounded connection. When the contact arms are in this position all voltages are grounded out. This position corresponds to the bow or stern aspect.

11. Y As the potentiometer arms are rotated away from the grounded center. taps the. voltage at the output arm increases at a geometric rate even though the potentiometers are linearV types. VAlso since the second potentiometer produces a loading ou the first potentiometer it makes it possible to alter the form of the resulting curve. To Ya fair approxi-mation thisv can bei adjusted to fit a tangentk curve. See FIG. 13. Y

Becausehi'ghest accuracy is desired in the vicinity of 45 the curve can be madecoincident with the tangent curvexin this region, allowing it to run out as the extreme positions are approached. When adjusting fora correct or'optirnum. ratio it is not necessary to employ potentiometers of diierent values. Both potentiometers can be; of the same value for standardizing purposesand a xed resistor 98 shunted across the second potentiometer. This fixed resistor accomplishes `the desired loadingV and alters. the curve shape.V Y

Errorsv can be rninimizedYY in the Y45 vicinity so that aspect errors will-be. less. than 1 and increasing either way out to values in the neighborhood of 5.Y or- %4 towards the ends. Y Y Y The'rst potentiometer is. excited push-pull sorthat Y when the arm` crosses the gap the 'reverse polarity is available. This gives the correct aspect voltage orientation when the ship passes through )beam aspect. Refer to- FIG. 10'. The opening ofthe circuit during the gap line. of, the target and toaalimited distance; n

because the aspect deflectionwave form voltage.wllicll'. v K

due toY its straight line- Ycharacteristic. forr target-V aspect, can position, signals just preceding; or.; following the target; only onVA the same.. straight line` The fact that'A it hast limited duration, limits correspondingly the lengthot Y the wake signal., This limitation. may.; not, beserious `since' most target wakes unless in -a bow or stern aspectA Y soon would run off the limited sector. width. The factY that target wake mayY be placedbefore or after the. target interest. Y

interval removes the aspect voltage and this nicely cor-V responds to the actual desired' beam situation. On either side of the gap' the voltage'will Vbe aV maximum vwhich gradually decreases as the center tapis approached. At

but with opposite polarity. This again'corresponds toy the desired characteristic. `as shown onFIG. 10..- It might be pointed out that if the duration of theV target echo pulse varies it will not attect the aspect. The only result will be the brightening of the aspect linefor a greater or less extent symmetricallyrabout the center position. v

Theoutputof potentiometer 94 is connected .to potentiometer 95 which is driven as a functionof range from. range servo box '72. l voltage with range to correspond with. the reduction of the deectionl ability as range increases.L The arm. ofpotentiometer 95 is. connected to theV grid*y of phase in.- verter 96 which convertsV the aspect deflection voltage to a push-pull voltage for proper drivecf the left and right phase shifter circuits. The resultingz phase modulation by means. of the target. aspect dellectionvoltaget has.Y been controlled in terms-ofY polarity andjamplitude. as a function Yof target aspect and range. Y

In the target 4aspect deflection generator iny box V89,Y two cam-operated switches 103 and-104cm driven,by,

target aspect servo motor inbox 106 which also drives aspect potentiometers 93 and 94 and potentiometer 91 in the Z voltage generator box 76. Switch 103 connects the grid of wake gate envelopev tube 108 inbox vZZ to the ends of the winding of potentiometer 931 The cam is arranged to switch the polarity'of the Z voltage fedY to the wake gate envelope tube 108 when the arm ofv the potentiometer passesover the gap at the ends of the winding. Y

Thus with one polarity the'po'sitive side ofthe Z voltL age will be theV first halfcycle while with the reverse polarity the second half cycle will be the positive side. The wake gate envelope tube 'is biasedltopass only the Y positiveV half cycle and thus its output contains a positive pulse only. For the rst position this pulse precedesA the targetl and for the second posi-tionk the pulse follows the target. This pulse thus can be used as the wake envelopel and presents the wake yin its fore or aft' position as the targetv swings throughbeam aspect.

The simulation of target wake is elected with some limitations. Two limitations areposition andA length;

The wake can be positioned only straight back alongYYthe Cam switchv 104V switches, on the. target'depthvv echo i envelope in; target depth, echov envelope box 3.0l lwhen'the. target` is inbeam aSPect. It switches` olthe depth. echo envelopefor all other aspect positions.

' The linear lsawtooth voltage taken 'fromftlierplate of the sawtooth switch tube 86 in the target- Z voltage gen-,YV

erator is placed on the; grid Yof' depthechoY pulse tube 112'..v

' This tube has a variable. positioncathode biasjobtainedl Y `by a bleeder from-B+., The cathode voltageof tube `112 is controlled by target depth potentiometer 11Std which the tube cathode is connected. Depth echo pulse isf aY Y delayed pulse subsequent to the target echo. Time delay isf determined when the sawtooth voltage has. sullicient` amplitude to cause the tube. to conduct withkithe given cathode bias setting as determinedI by .the depth echo,

Ypotentiometer 113. The amount ofltinie-fdelayis a function of' the DC; voltage/from the potentiometer 113 whichis driven as aV function of target depth; VAs previously mentioned Ythe sawtoothjvoltage `VandV4 the. poten-VV i tiomet'ervoltage are sorproportioned'that, zero depthposi- Y tionrgivesaQpul'se coincident with. ,that of' the targe.t,

Y IncreasesV in depth wouldincreasingly Ydelfaythe'coin-V 0f-other end of' which isfgrou'nded.V Resistors' 126 and 128"Y connected in series from Belr to ground in lead; 129 for-1n Y Itfreduces the aspect deflection?V cidence pulse` up tothe limit/of "the sawtooth voltage. A pulse transformer 1 14'is provided inthe plate circuit of tubeV 11:2*` toV shape .the initial plate currentllow into a pulse. Transformer output :is connected-[to a Ycathode follower comprising tube 116 the of which is connected to theseconda'ryof the transformer, `the a positive bias forvthezcathode` of cathode' follower 1116. The cathode follower'thus is biasedto clipLoff transient The'v cathode ofvk tube;

the depth echopulse on o r olif' The* output' ofi-tube 11 is fedto the-target envelopes` gate in box 195@ tliattht.j 1 ktargetldepth echo-ipulsemaybe'gated on and ol'wi'tlr Y thetargetenvelope in-t-hezfourtransducer channels.Y The targetV gate inbox 18 being connected t-or theoutput of" the gate in box 19,V thetargetsignal is gated-5to thel channels inaccordance with the depth? eel'loy pulse `as well `as the envelope pulse Vand',transducertrain and tilt-'f` Y error. Y t It is accordinglyseen. lziowfv theI target,` control* multi-l vibrator furnishes the target depth echo and-target wake pulsesy inl proper time .relation totheft'argetv pulse4 and how the-aspect- Vdeflection: voltagev isLder'i-vedv Yfrom ytheou'tputaof,the-multivibrator.. Y

Returning to the Z. voltage:.generatorthel outputizvoltY Y ager taken from: the. armioli.potentioi'meterQlisnusectftory v Y form the. target. envelope. :The center 'tap'roftluefporten#V Y tiometer winding i's tiedtto the: common cathode ofttubes..

' 81 and 90. and its arm: is servoedzasr a'functim Y aspect. ThisZ voltagefis fed to thev grid;- of. a two tube;- zerol grid cur-rent symmetrical limiter consisting; of tubes 130 and? 17316.` The biasron `the. grid of tube-130 isv adjusted by potentiometer ,132 while potentiometer- 1321,.

adjusts the grid of limiter tube .136,thus allowing sepa-l ate1 adjustment. of the positive. andv negative clipping4 eve i i These clipping levels are set for symmetricalclipping off the Z voltage andi'are notyaried Asub'sequently vduring operation. The input voltage" to cli'pper'is"v 13 varied in amplitude by the aspect potentiometer 91 as ahmction of aspect. When the voltage is large the clipping is deep and the wave form more square while with a low voltage the clipping is slight and the center transition slope more gradual. See FIG. 9b.

The output of limiter tube 136 is fed to a two stage RC differentiating circuit 140 comprising series capacitor 142 and grounded resistor 144 in the first stage and series capacitor 148 and shunt resistor 146 in the second stage. 'Ihe s'econd filter section while of the same time constant as the first has a considerably higher impedance to give sharper cut-off and lless amplitude loss. The shunt resistor 147 across the second differentiating capacitor 148 is to adjust the phase of the vfrequency components of the resulting pulse for better symmetry.

Dilerentiating the clipped wave form which has three vertical transitions the beginning down, the center slope up, and the end down, results in three pulses, the rst down, the second up, and the third down. Their durations correspond to the duration of their vertical transitions. See FIG. 9a which shows the sequence of these Wave forms and the effect amplitude variations has on the slope and duration of the center transition.

As a result of these relationships varying the amplitude of the input voltage to the clipper effects a corresponding variation in the duration of the center pulse. Also since the Z wave slope is essentially made up of straight lines the duration of the resulting pulse will be inversely proportioned to the clipper input voltage amplitude.

lThe dilerentiated clipped Wave has another inherent characteristic in that the amplitude of the resulting pulse is a function of the slope of the voltage transition. This gives tov the center pulse a varying amplitude depending upon steepnessV of transition slope. The steep slope thus has Aa short duration and produces a high amplitude pulse while the lesser slope has a long duration and a correspondingly low amplitude pulse. This matches actual conditions of echo amplitude or intensity in which target beam position gives a high intensity but a short duration of echo and a bow or stern aspect a lower intensity but a greater duration of echo.

A dualV triode tube 152 and 154 receives the output of the RC diiferentiating circuit on the grid of tube 152. Tube 154 is associated with tube 152 by means of a common cathode connection 155. Tube 154 has its grid biased to effect negative clipping. The dual triode tube is used to clip oif the negative leading and trailing pulses of the differentiated wave form leaving the positive one which is employed as the target envelope. Wave form F FIG. 9a. The target envelope pulse is `fed to the target envelopes gate in box 19 which is connected to the target gate in box 18 to gate on the target signal in the proper time relationship from the plate of triode tube 154 in the target envelope generator box 78.

I The outstanding feature of all of this circuitry is that only one source controls the entire associated functions of the target, such as aspect, wake, depth echo, and intensity variations. The functions derive naturally from the circuits and no oscillator or multivibrators are used,

which might affect individual accuracies or give rise to irregularities. Also since the functions relate to one source only,ldifferential inaccuracies are non-existent.

The circuitry for the phase Shifters shown in block 52 and block 150 of FIG. 1 and FIG. la respectively, is deemed a unique improvement over devices presently in use. As was previously explained the relative phases of the target and wake signals in the four transducer channels are. responsive to transducer train and tilt angleerrors and target aspect. A D.C. bias voltage controls the phase as a function of off-train errors and upon this bias is .superimposed the A.C. deflection wave form which describes target and wake aspect.

As shown in FIG. 4 the two outputs of rectifier tubes 4() and 41 represent dilerentially the transducer train angle error -as left and right. The same is true for tilt angle errors which represent top and bottom. However since the four quadrants have positions which are intermediate between right and left and top and bottom the developed error voltages have to be combined so as to be proper and equivalent for the four transducer channels.

. An arrangement for doing this is shown in FIG. 2. There is provided a diamond-shape arrangement of eight equal resistors with two to a side. Resistors and 161 are connected to the bottom left transducer channel; resistors 162 and 163 are connected to the bottom right transducer channel; resistors 164 and 165 are connected to the top right transducer channel and resistors 166 and 167 to the top left transducer channel. The intermediate D.C. biases from the junctions of the two resistors on a side are fed to the appropriate transducer channels. The left and right points of the diamond are fed with the left and right error bias voltages as derived from tubes 40 and 41 and the top and bottom points are fed with the top and bottom error bias voltages from tilt error rectifier tubes (not shown). Connected to the left hand transducer inputs in advance of the phase Shifters are capacitors 170 and 171. To the right hand transducer inputs are connected capacitors 173 and 174. Through capacitors 170 and 171 the left A.C. aspect deection voltage from phase inverter tube 96 shown in FIG. 1l is introduced while the right aspect deection voltage is introduced through capacitors 173 and 174. The capacitor connections in no way disturb the biases since the capacitors cannot pass D.C. and therefore produce loading. At the same time the resistors have suicient impedance so that the A.C. source is not excessively loaded. The circuit is actually similar to a resistance capacitor coupling as commonly employed in audio amplifiers. This A.C. aspect deflection voltage has to be supplied push-pull from a phase inverter tube as previously pointed out. Push-pull is required since the phase must be :retarded in one half while it is advanced in the other.

The phase shifter circuits are especially designed to give plus and minus 90 phase shift which correspond to the full grid swing of the phase shifter tubes, from cutoif to zero bias. It is important that the grid swing of the phase shifter tubes should be limited so that the phase shifting does not exceed the plus and minus 90 as otherwise the AN/SQG-O will begin to repeat the target display. A bias limit must also be present to prevent grid current in the phase shifter tubes which would a`ect the position bias and introduce errors. Accordingly deflection limiters in block 175 are provided to prevent the phase shifter grids from being overswung.

The limiter circuit consists of a diode in series with the grid of a cathode follower in each transducer channel. For example, triode 176 and cathode follower 177 are so connected in the top left channel; triode 178 and cathode follower 179 are so connected in the top right.

channel; triode 180 and cathode follower 181 are like- Wise connected in the bottom right channel and triode 182 and cathode follower 183 are connected as such in the bottom left channel. The triodes 176, 178, 180, 182, have their plates connected to the cathode follower grids in the Vabove arrangement with grid leak resistors 184, 185, 186 and 187, respectively in each combination tying the cathode follower grids to ground reference.

The action of the limiter circuits can be explained in.

the following manner. Consider first a signal excursion in the positive direction. This naturally carries the cathode of the diode with it and since the plate of the diode is at ground the diode ceases to conduct when the cathode reaches this potential. This opens the diode circuit and more positive signal swings cannot be passed on to the cathode follower grid. Thus the positive signal swing limit obtainable from the cathode follower is set. If signal swings in the negative direction are now considered we see that the diode will still continue to conduct carrying the diode plate and cathode follower grid along with it. Eventually the cathode follower will be cut off by its dividedtwo ways.

The voltage limit levelV out of the cathode follower Y will therefore be zero volts for the negative swings and a positive limit on positive swings determined by the positive cathodevoltage obtaining at zero gridv voltage.

This positive voltage at the cathode will be thel positive l limit. LtA should be noted that this can be. adjusted inde-v.

pendently of the input signal by the choice of; cathode follower plate, voltage and/or cathode resistor value. It will also be noted that the D.C. bias voltages have been offset and this it will be seen, is necessary for Afitting properly the phase shifter grid swing characteristic.

The phase shifter circuitry itself is interesting and is rather unique in that it develops a very large linear phase swing and onlyV alimited amount of amplitude variation. Tov significantly vary the output voltage with phase modulation, would seriously impair the value. of the phase shifter. j g f Y As shownV in FIG. 2 :a dualgtriode tubeis lprovidedfor each channel comprising triode phase inverters 190, 191,y 192 and 193 andtriode'phase Shifters 195, 196, 197 and 198. The phase inverters have equal load resistors inV the plate and cathode; The phase shifter tube has its cathode connected through `a quadrature capacitor 200, 201, 202 andV 203 to the plate of the phase inverter. A high value resistor 214, 216, 218, 220 from B+ to the plate ofthephase shifting tube is provided forV polarizing purposes. Phase shifting control voltage is fed from the deflection limiter cathode in series with the secondary of transformers 204, 205, 206, V207 to the grid of the phase shifter tubes. VTarget and wake signals are fed to the grids of the phase inverter tubes, 190, 191,v 192 andV 193 through capacitor and resistance couplings 222, 224, 226 and 228, respectively/,wand also to the primary of transformers 204, 205, 206 and 207. The platev resistance of the phase Shifters is controlled by the phase shiftingv Y modulating voltages placed on their grids from the. deflec-v tion limiters, inV series with the transformer secondaries.

The value of the phase. shifter plate resistance is of course limited by cut-off bias of the tube forthe negative swing and zero grid bias of the tube which is the maximum achieved voltage on the positive swing. Phase shifting circuits following this general form are capable of a maximum phase swing of 180 or plus-or minus 90?.v pro.- viding the Variable resistance can vary Vfrom zero to infinity. Since this is not possible with the phase'shifter Y tube less than this phase swing normally obtains. In order to have the phase shifter tube act as a pure variable resistance its grid musty be fed the same signal, equal in phase and amplitude, as its cathode.' The use of the transformer enables this to be done without interfering with the action of the modulating voltage especially the. higher modulating frequencies. By differentially adjust-4 the device is' adjusted for plus -and minus 90"V of phase modulation, however, an amplitude `modulation of about 30% will normally follow. Y This variation is symmetricalwith minimum amplitude at the center phase position and increasing evenly with phase rotation either way.

The plate circuit of each phase shifter is capacity cou-- pled to an isolating cathode follower, the cathode followers being numbered respectively in the four channels from left to rightl 230, 231, 232. and 233.. This enhances. stability of performance in thephase Shifters and reducesy the 4effect ofthe output loading on their operation. The coupling capacitors are purposely keptsmall so that low frequency modulating components would be discriminated against. p

As explained the output A One branch feeds the individual targetV gate 18 and the other the reverberation modulator 20.

of Ythe V noise lmodulator 16 is This second modulator modulates thesignaly withgaverylow band of random noisel frequencies, seletedbyrthegz very low-pass filter. 23 from thesame Original random.; This giyeste thsbranch ofthe signalV i an envelope characteristicrepresentativeof reverberations..

noise source tube.

. Output, fromthe 'modulator 20. is furthenrsubdvided.;

Y One branch feeds Vingliyidual,wake. gate ZL'ABQJlen Y bnanch appropriately yattenuated withv timeY pt sition-` effects, furnishes Vreverberation signals.v A manual` at;

tenuator for these reverberation signalsrallows Y Vsimulate various searstate condi-tions.

For adaptation wtaef'AN/sQo-t )antennas adi-' rectional transducer, thefreverberation intensity is. varied as a functionofangleof trainfV yAgain Qontrol 'sion angleV is increased. This would bethe. equivalentof training under own ships wake and surface;reverberations. TheseV controls for reverberation signals are. effected in diagram.Y Y

Y In this relatively simplelmaimf'we dispose: 0f.

problem of. reverberatiom sea state orV vsurface.,reyerheration, and own ships wake. The simulation also would quite representative from the operational ,viexizpoint and.

rteristics which closely 'match actual.- signals.'v Y Reverberations arrive from all,Y directions. equallyjenar, cept as vpreviously noted for` surface rever-berations. t

most importantlythe signalI itself would characf Here an` intensity change Yas afunction of'tilt anglep Y vides. the. appropriate` directional infomation. Howevenf.

7 theiappearance ofthe. reverberations onV the... scopes, due.; to the factl .that reverberationsreturn from; randomA sc :at- VVters, randomly located either side of the. .directionof4 scan. This means. the phase ofthe reverberationsignals' in; each transducer is. notidentical butdivfferent, d epexldingr.'VV uponther location of the Scatters.. Two phase shi-liters. ingv box 52 sare fedin push-pull with a random noise voltarge obtained-byV selectingl a: suitable frequency band .fromthe l random noise generator` in box `This differentially shifts thev` phase of. the reverberation one; random:- basis,v resulting inl-a lateral Spreading ofzthe. reverberation,

signal onine. aammhseepejQf-the YAISI/Societ l g). Nc.L means of giving-.a spreadin the...verticalIV direction as displayed on the? depthvseoperis illustrated,

However, by repeating the Vsame .process and.differentiallyxv phase modulating the two vertical of thetransndusl inputs aspread ofjthe.vr reverb,erations.YoIfLtllei will fbe obtained. Y,

The outputvof the. cathodetfollowes thereverberation echoes fromV block. 51 areY then fedto range attenuation`V amplifiers in` box 210 where 4relative.

intensities. of all the signalsaresimultaneouslycontrolledA and thus their relative amplitudes preserved.. A single.

range attenuatoravoids;calibratingfrange attexlllzltion.V

characteristics between .different signals forY of trackingi.. The range Vattenuator iSlv colltrolledv as afunc.-y tionof dynamic ranger; Target pulses are. correlated, through the range attenuator with the. transmitterfon and off controlin the: operational gear. i Y i Signals representing yexternal noises land sounds Vsuch as from own shipspropellermay belgeneratect'bysut able circuitry in block 212. j Propelernoise amustbe'lr Vgated tofpass to thefchannelswhen thevtransducerls pointed aft and therefore aY position'gat'e 1s proxnjddl which is .driven as 'av function of tilt bearingangles: Since the distance of thelnoisesoundf isconstant` napro-1 viSiOl-l .lsimd for range attenuation. The output of Vreverberation control box 50in. the block;`

17 block 212 is introduced to the channels after the range attenuator 210.

In order to'adjust the signal outputs of the simulator an output attenuator 214:1 is provided. This enables a suitable signal level to `be provided to the AN/SQG-() sonar transducer input circuits.

What is claimed is: t 4 l 1. In a sonar simulator for a sonic device a signal frequency oscillator, means for modifying the frequency of said oscillator to simulate the eifect of doppler of own ship and .target comprising a reactance doppler modulator connected to said oscillator and adapted to shift the frequency of the oscillator, high impedance voltage source supplying to said reactance doppler modulator a voltage proportionate to a simulated own ships speed, means for modifying said voltage as a function of a simulated transducer train angle, low impedance means for supplying to said reactance doppler modulator a voltage proportionate to a simulated relative target speed, a target envelope clamp circuit connected between said low impedance means and said reactance doppler modulator, said clamp circuit being operated by a target envelope volta-ge whereby the simulated relative target speed voltage is applied to the reactance doppler modulator for the duration of the target envelope voltage.

2. In a sonar simulator for a sonic device as claimed in claim 1 wherein there is provided a target envelope gate connected to the clamp circuit, the target envelope voltage being passed through the target envelope gate to the clamp circuit, said gate being operated as a function of the simulated training direction of the sonic device.

3. In a sonar simulator a target control simulator system comprising a multivibrator adapted to be triggered by a range coincidence pulse to generate a negative pulse of substantially long duration, a sawtooth wave switch tube connected to the output of said multivibrator for generating a sawt-ooth voltage for the duration of the negative multivibrator voltage output, a Z voltage generator connected to said multivibrator and said sawtooth generator and adapted to receive .the negative voltage output of the multivibrator and the said sawtooth voltage of the sawtooth generator whereby the two volt-ages are combined to produce a Z voltage output and bias means applied to said Z voltage generator to adjust the symmetry of the Z voltage output.

4. A target aspect wave form generator comprising a phase inverter, means for supplying a Z voltage to said phase inverter, a pair of linear, cascaded potentiometers connected to the output of said phase inverter, said potentiometers having the centerpoint of the windings grounded, the rst potentiometer having its terminals connected lto the push-pull output of said phase inverter, the second potentiometer having its terminals connected together and to the arm of said first potentiometer, and a resistor connected to the arm of said first potentiometer and ground, the -arms of said first and second potentiometers being mechanically coupled together in corresponding positions and driven as a function of simulated target aspect, a variable potentiometer having one terminal connected to ground and the other terminal connected to the -arm of said second potentiometer, the arm of said variable potentiometer being driven as a function of simulated target range and furnishing the simulated target aspect output voltage.

5. In a sonar simulator Ea target envelope generato-r comprising a potentiometer, said potentiometer being driven as a function of simulated target aspect, means for producing a Z voltage connected to the input of said potentiometer, a limiter circuit connected to the output of said potentiometer and provided with means for producing positive and negative clipping of the aspect controlled Z voltage, differentiating means connected to the output of said limiter and adapted to differentiate the clipped output wave form producing three differentiated pulses, the center pulse having an opposite polarity to that of the J18 other two pulses and a clipping means connected to the output of said differentiating circuits and adapted to select the center pulse. l

6. In a sonar simulator a target depth echo generating system, including a Z voltage generator having a sawtooth generator, a delayed coincidence circuit having its input connected -to said sawtooth voltage generator, a potentiometer driven as 'a function of simulated target depth and arranged to vary the bias on the delayed coincidence circuit such that the coincidence will be caused to loccur from the center of the sawtooth voltage to the extreme end thereof, a switch adapted to be driven as a function of simulated target aspect and connected to said coincidence circuit, the switch connection having means for opening the coincidence pulse output when the simulated target aspect is near beam position and blocking said output when the simulated target aspect is in any other position, whereby the coincidence pulse output is caused to appear only in the vicinity of the simulated target beam aspect.

7. In a sonar simulator a target characteristic control system comprising a multivibrator triggered by a target range coincidence pulse, a sawtooth generator controlled by said multivibrator, a target depth echo system connected to said sawtooth generator and adapted to develop a target depth echo pulse as a function of simulated target depth land simulated target aspect, a means of combining said multivibrator and sawtooth generator outputs to form a Z voltage, a target aspect generator connected to said Z voltage producing means, a target wake envelope generator also connected to said Z voltage producing means, said target aspect control voltage and wake envelope generators being adapted respectively to develop a target aspect control voltage as a function of simulated target aspect and simulated target range and a target wake envelope voltage as a function of simulated target aspect, means for varying said Z voltage in accordance with said simulated target aspect, a target envelope generator system connected to the last mentioned means and adapted to produce a target envelope pulse varying in duration as a function of simulated target aspect.

8. A sonar simulator comprising a signal source oscillator, a random -noise generator, a noise modulator connected to the output of said oscillator and said random noise generator, a target gate connected to said modulator, a target phase shifting circuit connected to said target gate, a limiter circuit connected to said phase shifting circuit, a wake gate connected to said phase shifting circuit, a target envelopes gate connected to said target gate, a target characteristics control system including a target depth echo envelope generator, a target envelope generator, a target wake envelope generator, and a target aspect deflection generator, said target aspect deliection generator lbeing connected to said limiter circuit, said target depth echo envelope Vgenerator and said target envelope generator being connected to said target envelopes gate, a target doppler clamp connected to said target envelopes gate, a reactance doppler modulator connected to said target doppler clamp and to said oscillator, high impedance means for supplying a voltage to said reactance modulator proportionate to simulated own ships speed, low impedance means for supplying a voltage to said target doppler clamp proportionate to simulated relative target speed, means for introducing a voltage proportionate to simulated target depth to said target depth echo envelope generator, means for introducing -a voltage which is a function of simulated Itarget position training to said wake gate and said target envelopes gate, and said target envelopes gate, and training error voltages to said limiter circuit, means for introducing a voltage which is a function of simulated target aspect and target range to the limitor circuit and means for controlling the noise modulator as a function of ping length.

9. In a sonar simulator, an echo signal characteristic simulator comprising a target signal circuit, a reverberaquency source sha-red by'eavch. off s'aid"` Circlts-wh'by the same frequency is necessarily impressed''onV thev vtW circuits,` a random noise source and aV noise modulator disposed in said circuits, the' input of said noise :nodu-Y Vlator being connected to saicl single; frquncyf srr'u'rcc v1.0. In asonar simulatnian echo signal -chctri'stic 

